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Minimum weight design of an axially compressed isotropic prismatic panel consisting of a series of cylindrical segments and verification by STAGS David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303 Michael S. Jacoby, Lockheed Martin Missiles and Space, Palo Alto, California 94304

David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

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Minimum weight design of an axially compressed isotropic prismatic panel consisting of a series of cylindrical segments and verification by STAGS. David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303 - PowerPoint PPT Presentation

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Page 1: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Minimum weight design of an axially compressed isotropic prismatic panel

consisting of a series of cylindrical segments and verification by STAGS

David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California

94303

Michael S. Jacoby, Lockheed Martin Missiles and Space, Palo Alto, California

94304

Page 2: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Optimized design of the type of corrugated panel studied

Page 3: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Summary• What is GENOPT? (Slides 4 - 17)• What is BIGBOSOR4? (Slides 18 and 19)• Problem formulation (Slides 20 and 21)• Geometry (Slides 2, 23, 29, 38 - 44 )• Objective versus design iterations for SUPEROPT execution (Slide 22)• Buckling modes and eigenvalues from GENOPT/BIGBOSOR4 (Slides 30-32)• Design Sensitivity of the optimized tank/strut system (Slides 33 & 34)• What is STAGS (Slide 35)• STAGS model and predictions from STAGS (Slides 36 & 37)• Comparison STAGS and GENOPT/BIGBOSOR4 results (Slide 37)• Extension of GENOPT/BIGBOSOR4 model to wide panels (Slides 38-43)• Optimization of panels with major segments and sub-segments (Slides 44, 45)• Smoothing away the “corners” (Slides 46 - 51)• Optimized panels that can be fabricated by stamping (Slide 52)• Corrugated panel mapped onto a cylindrical surface (Slides 53 - 55 and 61) • Externally T-stringer-stiffened cylindrical shell optimized by PANDA2 (56,57)• Optimization of a cylindrical shell with a truss-core sandwich wall (58, 59, 60)• Conclusions (Slides 80 - 83)

Page 4: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 5: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 6: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 7: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 8: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 9: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 10: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 11: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 12: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 13: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 14: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 15: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 16: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 17: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303
Page 18: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

What is BIGBOSOR4?

• Stress, buckling and vibration of elastic shells of revolution (BIGBOSOR4=BOSOR4 with more shell segments permitted, up to 295 shell segments as of 2011).

• Buckling of segmented prismatic panels such as that just shown.

• New version of BIGBOSOR4 called “HUGEBOSOR4” which will handle up to 2950 shell segments as of September, 2013.

Page 19: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Matrices governing vibration and buckling of shells of revolution derived via BIGBOSOR4 are narrowly banded

Page 20: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

The prismatic corrugated panel is optimized subject to the following “behavioral” constraints:

• Local buckling that is symmetric about the symmetry plane at x = WIDTH/2

• General buckling that is symmetric about the symmetry plane at x = WIDTH/2.

• General buckling that is anti-symmetric about the symmetry plane at x = WIDTH/2.

• "Classical" buckling of each cylindrical segment of the corrugated panel including a suitable knockdown factor from 1975 book by Brush and Almroth.

• Maximum allowable stress

Page 21: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

The objective is:

• Objective= WEIGHT (lb) of the entire panel of WIDTH = X inches

Page 22: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Evolution of the objective (panel weight) during a single execution of SUPEROPT

Page 23: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Starting and optimized design of a panel with 5 “convex up” segments over WIDTH/2 = 50 inches

Page 24: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Typical design margins of an optimized design:MARGINS CORRESPONDING TO CURRENT DESIGN (F.S.= FACTOR OF SAFETY)MARGIN CURRENT NO. VALUE DEFINITION 1 9.540E-02 6.05-0.10*V(6)-0.10*V(7)-0.10*V(8)-0.10*V(9)-0.10*V(10)-1 2 4.600E-03 -3.95+0.10*V(6)+0.10*V(7)+0.10*V(8)+0.10*V(9)+0.10*V(10)-1 3 5.380E-03 (LOCBUK(1)/LOCBUKA(1))/LOCBUKF(1)-1;F.S.=2.00 4 2.171E-03 (BUKSYM(1)/BUKSYMA(1))/BUKSYMF(1)-1;F.S.=1.50 5 8.285E-03 (BUKASY(1)/BUKASYA(1))/BUKASYF(1)-1;F.S.=1.50 6 8.958E-03 (CYLBUK(1,1 )/CYLBUKA(1,1))/CYLBUKF(1,1)-1;F.S.=1.0 7 5.542E-01 (CYLBUK(1,2 )/CYLBUKA(1,2))/CYLBUKF(1,2)-1;F.S.=1.0 8 8.370E-02 (CYLBUK(1,3 )/CYLBUKA(1,3))/CYLBUKF(1,3)-1;F.S.=1.0 9 5.350E-02 (CYLBUK(1,4 )/CYLBUKA(1,4))/CYLBUKF(1,4)-1;F.S.=1.010 2.183E-02 (CYLBUK(1,5 )/CYLBUKA(1,5))/CYLBUKF(1,5)-1;F.S.=1.011 2.057E+00 (STRESSA(1)/STRESS(1))/STRESSF(1)-1; F.S.= 1.50

LOCBUK means local buckling load factor.BUKSYM means symmetric general buckling (buckling mode issymmetric about the symmetry plane).BUKASY means anti-symmetric general buckling (buckling modeis anti-symmetric about the symmetry plane).CYLBUK means knocked down “classical” buckling load factor:buckling of each cylindrical segment from classical theoryincluding the appropriate knockdown factor

Page 25: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

“Classical” buckling knockdown curve, “A design recommendation” from Brush & Almroth (1975)

Page 26: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Decision variable candidates (1 of 3)

Page 27: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Decision variable candidates (2 of 3)

Page 28: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Decision variable candidates (3 of 3)

Page 29: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Optimized cross section profile for the specific case, “fold98updown”

Page 30: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Anti-symmetric general buckling of the optimized panel cross section profile

Page 31: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Symmetric general buckling of the optimized panel cross section profile

Page 32: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Local buckling of the optimized cross section profile

Page 33: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Design sensitivity of optimized “fold98updown” panel with respect to YPLATE(8)

Page 34: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Design sensitivity of optimized “fold98updown” panel with respect to YPLATE(9)

Page 35: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

What is STAGS?• STAGS [16 -19] is a finite element code for the general-purpose

nonlinear analysis of stiffened shell structures of arbitrary shape and complexity. Its capabilities include stress, stability, vibration, and transient analyses with both material and geometric nonlinearities permitted in all analysis types. A large rotation algorithm that is independent of the finite element library has been incorporated into STAGS. Solution control in nonlinear problems includes specification of load levels or use of the advanced Riks-Crisfield path parameter that enables traversal of limit points into the post-buckling regime. Two load systems with different histories (Load Sets A and B) can be defined and controlled separately during the solution process. Imperfections can be generated by superposition of several buckling modes determined from previous STAGS analyses of a given case. “Shell units” can be modeled with minimal user input as individual substructures in which the analytic geometry is represented exactly. Complex structures can be assembled from multiple relatively simple shell units or from a finite element unit.

Page 36: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

STAGS model of half the width of the previously optimized “fold98updown” panel cross section profile

Page 37: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Critical buckling mode & load factor from the STAGS model

Page 38: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Optimized “fold98updown” profile with changed left-hand boundary condition

Page 39: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Extension of BIGBOSOR4 model to the full width of the optimized panel

Page 40: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Extension of BIGBOSOR4 model to a wide panel with 5 full widths of the new optimized profile

Page 41: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Optimization of corrugated panels with uniform “up-down” segments

Page 42: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Extension of previously optimized “uniform curved” panel to wide “curved” panel

Page 43: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Extension of previously optimized “uniform flat” panel to wide “flat” panel

Page 44: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Optimization of a panel with both major segments and sub-segments

Page 45: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Comparison of optimized panel cross section profiles for panel with sub-segments

and panel with no sub-segments

Page 46: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Smoothing away the “corners”

Page 47: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Zoomed view of one smoothing segment

Page 48: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Cross section before and after smoothing

Page 49: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Buckling load factor versus RSMOOTH

Page 50: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Optimizing a cross section with a smoothed profile

Page 51: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Extending the optimized profile to that of a wide panel with reflected and

repeating profiles

Page 52: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Optimization of a panel that can be fabricated by stamping

Page 53: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

An optimized multi-WIDTH “flat” panel mapped onto a cylindrical shell

Page 54: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

The first eigenvector and eigenvalue of the cylindrical shell (left) and the critical (1st

eigenvector and eigenvalue) of the equivalent “flat” panel (right)

Page 55: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

General buckling of a complete cylindrical shells with (left side) MMM = 6, RCYL = 95.493 inches and (right side) MMM=18, RCYL=286.48 inches

Page 56: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

General buckling of optimized externally T-stringer-stiffened cylindrical shell optimized by PANDA2

Page 57: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Two more critical buckling modes of the optimized T-stiffened shell

Page 58: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

General buckling from BIGBOSOR4 of an optimized cylindrical shell with a truss-core sandwich wall

Page 59: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

General buckling of the optimized truss-core sandwich panel from STAGS

Page 60: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

General buckling of an optimized cylindrical shell with a truss-core sandwich wall (HUGEBOSOR4 model)

Page 61: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

HUGEBOSOR4 model of smoothed “fold916updwn” with 940 segments

Page 62: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Local buckling of an optimized cylindrical shell with a truss-core sandwich wall

Page 63: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Buckling of axially compressed optimized uniformly corrugated cylindrical shell

Page 64: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

BIGBOSOR4 and STAGS models of optimized complex corrugated cylindrical shell & buckling mode

Page 65: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

The WEIGHT of “global” optimum designs versus number of major segments over WIDTH/2=50 inches

Page 66: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Optimization of narrower panels

Page 67: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Re-optimization of the profile shown on the previous slide with corners (no smoothing)

Page 68: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

STAGS model of the same cross-section profile and prediction of buckling

Page 69: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Three “anti-symmetric” buckling modes

Page 70: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Configuration and buckling of the “best” complexly corrugated panel (smoothing is present)

Page 71: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

STAGS model and results (narw96updown with smoothing & 12 major segments spanning 50 inches)

Page 72: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

HUGEBOSOR4 model of 360-degree cylindrical shell: narw96updown with smoothing

Page 73: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

STAGS huge model and results. There are 2.2 million d.o.f. in this STAGS model

Page 74: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Configuration and buckling of the simplest optimized complexly corrugated panel:

narw91updown with 9 major segments spanning a width of 50 inches.

Page 75: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Configuration and buckling of the simplest optimized complexly corrugated panel: narw91updown with 9 major segments spanning a width of 50 inches. The

simple model is expanded and cylindrically mapped.This is a BIGBOSOR4 model

Page 76: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

STAGS narw91updown model and results

Page 77: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

A case for which the “852” optimization strategy followed by the “1532” strategy worked (case = fold914updwn)

Page 78: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

A case for which the “852” optimization strategy followed by the “1532” strategy did not work (case = fold913updwn)

Page 79: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

A huge model analyzed with HUGEBOSOR4

Page 80: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Conclusions (1 of 4)• Predictions from STAGS and from GENOPT/BIGBOSOR4 for optimized

corrugated panels (Figs. 20 – 22) agree well enough to justify the use of GENOPT/BIGBOSOR4 for obtaining optimum designs, provided that GENOPT/BIGBOSOR4 can produce an optimized weight that is reasonably close to that corresponding to a “global” optimum weight.

• Optimized panels with uniform alternating “convex surface up”/ “convex surface down” major cylindrical segments (fold98updwnu - Figs. 16 – 19) weigh significantly more than analogous optimized panels with alternating “convex surface up”/ “convex surface down” major cylindrical segments the geometry of which varies from segment to segment (fold98updown - Figs. 2 and 6 – 12). By “geometry” is meant cylindrical segment radius, subtended angle (2 x PHISEG), and orientation [YPLATE(i+1) – YPLATE(i)].

• In the two cases in which sub-segments are introduced (fold98supdwn – Figs. 13, 14, 15 and fold94S – Fig. A6) it is determined that there is no advantage of having corrugated panels with sub-segments.

Page 81: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Conclusions (2 of 4)• At least in two cases (fold98updown – Figs. 23a and 23b and fold916

– Fig. A10) some of the buckling margins for an optimized design are very sensitive to changes in one or more of the decision variables for values of those decision variables in the neighborhoods of the optimum values. It is likely that this characteristic makes it difficult to find “global” optimum designs, leading to a “jaggety” behavior of the objective from design iteration to iteration such as that exhibited for the specific case, fold98updown, in Fig. 26 and for the case, fold916, exhibited in Fig. A11(A).

• GENOPT/BIGBOSOR4 has difficulty determining “global” optimum designs for corrugated panel configurations with many major cylindrical segments. Optimization cycles from executions of SUPERDUPEROPT with multiple sequential executions of SUPEROPT often converge to designs of panels with weights that can be significantly higher than those of known “global” optimum designs. It is quite possible that the “response surface method” described in [10 - 15] would lead to optimum designs that weigh less.

Page 82: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Conclusions (3 of 4)• For the corrugated panels with overall dimensions 100 x 100 inches,

with all “convex surface up” cylindrical segments and with a relatively large number of major segments the optimized designs display merging of the major segments into fewer approximately cylindrical segments with larger radii. The optimized weights of these “convex surface up” corrugated panels are insensitive to the number of major segments for configurations with four to eight major segments over half the width of the panel (Fig. A5).

• A modification of the boundary condition along the left-hand longitudinal edge of a panel from “u,v,w held; rotation free” to “symmetry/anti-symmetry” leads to slightly heavier optimum designs (fold98updown – top frame of Fig. 9 compared to Fig. 6), but permits the post-optimization extension of the analysis by BIGBOSOR4 to wide panels with multiple repeating sections of width, WIDTH, (Figs. 10 – 12).

Page 83: David Bushnell, AIAA Fellow, 775 Northampton Drive, Palo Alto, California 94303

Conclusions (4 of 4)• “Smoothing” away the “corners” between adjacent major

segments and at the left-hand and right-hand longitudinal edges may have a significant influence on the minimum buckling load factor. This is so in the specific case called “fold98updown”, as demonstrated in Fig. 30.

• One can obtain optimized panel cross-section profiles that can be fabricated by stamping, as demonstrated in Fig. 32.

• An optimized corrugated cylindrical shell weighs significantly less than an optimized “equivalent” externally T-stringer-stiffened cylindrical shell or an optimized cylindrical shell with a truss-core sandwich wall (Figs. 33 – 37) and significantly less than an optimized cylindrical shell with uniform corrugations (Figs. 38 and 39).

• A “HUGEBOSOR4” has been created to handle up to 2950 shell segments, 10 times the maximum permitted with BIGBOSOR4.